EP4257929A1 - System zur messung einer physikalischen grösse und/oder positionsmesssystem mit bistablem magnetdraht sowie messverfahren - Google Patents

System zur messung einer physikalischen grösse und/oder positionsmesssystem mit bistablem magnetdraht sowie messverfahren Download PDF

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Publication number
EP4257929A1
EP4257929A1 EP22166892.4A EP22166892A EP4257929A1 EP 4257929 A1 EP4257929 A1 EP 4257929A1 EP 22166892 A EP22166892 A EP 22166892A EP 4257929 A1 EP4257929 A1 EP 4257929A1
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EP
European Patent Office
Prior art keywords
magnetic wire
bistable magnetic
bistable
measurement
physical quantity
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Pending
Application number
EP22166892.4A
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English (en)
French (fr)
Inventor
Rastislav VARGA
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Rvmagnetics AS
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Rvmagnetics AS
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Publication date
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Priority to EP22166892.4A priority Critical patent/EP4257929A1/de
Priority to PCT/IB2023/053187 priority patent/WO2023194852A1/en
Publication of EP4257929A1 publication Critical patent/EP4257929A1/de
Pending legal-status Critical Current

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/12—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
    • G01D5/14—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage
    • G01D5/142—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices
    • G01D5/147—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices influenced by the movement of a third element, the position of Hall device and the source of magnetic field being fixed in respect to each other
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00—Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42—Devices characterised by the use of electric or magnetic means
    • G01P3/44—Devices characterised by the use of electric or magnetic means for measuring angular speed
    • G01P3/48—Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage
    • G01P3/481—Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals
    • G01P3/4815—Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals using a pulse wire sensor, e.g. Wiegand wire

Definitions

  • the invention relates to a composition of excitation element and a bistable magnetic wire, where a composition is prepared for measuring of various physical quantities and/or for position measurement of the bistable magnetic wire.
  • the novelty of the system and method lies mainly in the specific asymmetrical position of a magnetic field of the excitation element and the actually bistable magnetic wire, thanks to which the interpretive value of the raw measured data is significantly improved.
  • bistable magnetic elements are used for measurement various physical quantities and position, where the bistable magnetic element is formed by a passive member which by its magnetization reacts to a change in position in the magnetic field or to a change in a physical quantity.
  • bistable magnetic properties An alloy with bistable magnetic properties and a micro wire from this alloy is described, for example, in document GB2374084A .
  • the micro wire is able to respond to various physical quantities, but response evaluation is problematic, because prior art bistable magnetic elements can have complex magnetic acts where the magnetization occurs in a multiple domains within a single micro wire, not a single wall jump.
  • Applications of bistable magnetic wires in position measurement, angular measurement and revolution measurement are also known.
  • DE2817169A1 , DE3427582A1 , SU1753425A1 describe systems with a Wiegand wire having a certain level of magnetic bistability, wherein these systems serve to determine the approximation of a bistable magnetic element to a sensor. Due to this arrangement, it is not possible for measurement the values of physical quantities in the vicinity of the bistable magnetic element.
  • the position sensor or rotation sensor according to publication EP0484716A1 uses the Wiegand wire to which rotating permanent magnets approach. The sensor responds only to changes of the magnetic field, it does not evaluate the size of physical quantities.
  • the Wiegand sensor according to document DE4107847C1 allows to contactlessly transfer the information about closure of the switch, which can react to the change in a physical quantity such as temperature, pressure, acceleration, but it requires an appropriate sensor by which subsequently the switch is controlled, i. e. the physical quantity is not measured by the bistable magnetic element itself.
  • bistable magnetic element itself has to react to the changes in the measured physical quantity and also generate a response, which is contactlessly transmitted to the receiving element.
  • a system for measuring a physical quantity and/or for position measurement with bistable magnetic wire where the system comprises the excitation element for generating a magnetic field within range of which the bistable magnetic wire is placed.
  • the bistable magnetic wire has a first end and an oppositely placed second end, therefore is not wound into a screw or coil, wherein the bistable magnetic wire is adjusted for magnetization by a single Barkhausen front jump from the first end to the second end or vice versa, according to this invention, the nature of which consists in that the excitation element and the bistable magnetic wire are placed in a mutual position in which the size of the magnetic field excited by the excitation element at the first end is different from the size of the magnetic field excited by the excitation element at the second end.
  • the magnetic field at the first end and at the second end is different in every moment of the non-zero excitation, thus at a given moment, wherein the excitation is dynamic in time.
  • the system also comprises a receiving element for response receiving from the bistable magnetic wire.
  • first and second in this document are used to name two ends differently, and these are interchangeable, thus the terms first and second does not express the superiority or importance of the respective end of the bistable magnetic wire.
  • the different magnetic field at the ends in given moment of excitation leads to an asymmetric magnetic field, which, together with magnetization by a single Barkhausen jump, leads to repeatable interpretable measurement results.
  • it is important that the behavior of the bistable magnetic wire is influenced fundamentally by the measured quantity or measured position, and that other factors, including acts of more complex magnetic properties of the bistable magnetic wire, were negligible or at least identifiable in a way that allows correction when evaluating raw data.
  • a difference of 5 %, preferably 10 %, especially preferably more than 25 % in the values of the magnetic field at the first end and at the second end is sufficient. This contributes to the magnetization taking place in one jump within the entire wire from one end to the other. If the magnetization took place within a number of separate domains along the length of the wire, the measured response would include a number of individual acts, which significantly impairs the interpretability of the measurement. It is not possible to subsequently identify the dependence of the measured data, which reduces the application possibilities of the bistable magnetic wire.
  • the aim of this invention is to achieve effective, thus complete, real bistability of magnetization, where the domain structure of the bistable magnetic wire does not consist of many domains, which would otherwise lead to magnetization by movement of multiple domains within a single wire.
  • the measurement of a bistable magnetic wire with multiple domains along its length can be compared to the measurement of several separate bistable magnetic wires in a single excitation field, what causes that the resulting measurement is a sum of individual responses that cannot be reliably identified and the summary response vector is therefore practically unusable.
  • the measurement of changes in the magnetic field allows to detect a change in position, a change in the rotation of the bistable magnetic wire or the carrier on which the bistable magnetic wire is mounted, and also allows to measure the relative position with respect to another object carrying the excitation element.
  • position sensors rotation sensors, end sensors, sensors of proximity of a magnetic object or carrier with a magnetic object, sensors of absolute position with respect to earth's magnetic field, and the like.
  • the antenna of the excitation element may be used for measurement the response, or preferably the system comprises a separate receiving element, for example in the form of a receiving coil.
  • the excitation element may be a primary coil, and the receiving element will be formed by a secondary coil.
  • the secondary coil can be connected to an amplifier and an evaluation unit.
  • the receiving element may be located coaxially with the position of the bistable magnetic wire or may be in another position mutual to each other so as to be within range to allow for response to be received.
  • the bistable magnetic wire is in the form of a micro wire with a diameter less than 50 ⁇ m, preferably less than 25 ⁇ m, especially preferably less than 15 ⁇ m. It is precisely at core diameters less than 15 ⁇ m and with suitable composition of the amorphous metal alloy, the radial magnetic structure disappears, which is related to the process of wire drawing with simultaneous rapid cooling, usually water cooling. Thanks to that the bistable magnetic wire behaves as fully bistable, thus effectively bistable over the entire length of the wire, and the domain wall during magnetization runs from the first end to the second end, not separately within several individual zones along the length of the wire. It has also been found suitable if the length of the bistable magnetic wire is at least 100 times, preferably at least 10000 times larger than the diameter of the bistable magnetic wire, which implies that it will be a small diameter wire, which we can also call micro wire.
  • a typical construction of the bistable magnetic wire includes an amorphous metal core and a cover, for example glass cover, whose outer diameter is no larger than three times the diameter of the metal core.
  • the thickness of the glass cover can range 1 to 20 ⁇ m.
  • the glass cover, glass surface layer protects the metal core from electrical contact with the environment, from aggressive chemical environment, thanks to which the bistable magnetic wire can be used very universally, for example directly in the electric motor windings or inside of building materials, inside of human body and the like.
  • a magnetic excitation with a triangular signal usually with a symmetrical triangular signal, which simplifies the evaluation of measured signal as described in older publications of the authors of this invention, has proven to be suitable.
  • the system according to this invention is adjusted to be connected to a power element, a control element and an evaluation element.
  • the power element transmits to the excitation element a power supply regulated to obtain a triangular excitation signal.
  • the evaluation element acquires and analyzes the response received from the bistable magnetic wire.
  • the asymmetry of the excitation field can be achieved in such a way that the excitation element, which induces a substantially symmetrical field, is arranged relatively asymmetrically with respect to the bistable magnetic wire.
  • positional asymmetry ensures that the first end of the bistable magnetic wire is in a higher magnetic field than the second end, and therefore the bistable magnetic wire will be magnetized always with movement of one domain wall, the one which is in the higher field.
  • Positional asymmetry can be achieved by setting a spatial relationship.
  • the coil of the excitation element and the bistable magnetic wire can be arranged coaxially, thus with identical or parallel-oriented longitudinal axes.
  • the asymmetry of the excitated magnetic field can be ensured by the construction of the excitation element with an uneven coil winding, for example with different thread pitches or with different number of threads at the first end or at the second end.
  • the result of such a construction of the excitation element is a different size of the magnetic field at the ends of the excitation element, or at a certain distance from these ends.
  • the mutual position of the excitation element and the bistable magnetic wire may be spatially symmetrical, but at the first end and at the second end of the bistable magnetic wire, it will be in a differently sized magnetic field.
  • the definition describing the mutual position of the excitation element and the bistable magnetic wire according to the first claim also includes a symmetrical mutual position if an asymmetrical magnetic field is generated by the excitation element.
  • the definition of the first claim expresses a mutual arrangement, which can be achieved by several means, or by a different combination of technical means and relative spatial arrangement.
  • the asymmetry of the magnetic field important to achieving the effects according to this invention is always understood in the relative relationship of the sizes of the magnetic field at the first end and at the second end.
  • the asymmetry of the excited magnetic field can also be achieved by adding a shielding element or by placing another, secondary coil to the primary coil to the primary coil of the excitation element. In such a case, the mutual position of the excitation element and the bistable magnetic wire may also appear to be spatially symmetrical, but the asymmetry of the magnetic field at the first end and at the second end will be important.
  • the excitation element can be placed coaxially with the position of the bistable magnetic wire or can be placed next to the bistable magnetic wire.
  • the longitudinal axis of the magnetic field generated by the excitation element will be essentially parallel to the longitudinal axis of the bistable magnetic wire, but in principle an angularly different position is also possible, for example, the longitudinal axis of the excitation element deviates from the longitudinal axis of the bistable magnetic wire within 30 degrees.
  • the disadvantages mentioned in the prior art are eliminated by the method for physical quantity measurement and/or for position measurement with the bistable magnetic wire, where a variable magnetic field is transmitted by the excitation element, wherein at least one bistable magnetic wire is placed within the range of the excited magnetic field, which is magnetized when the magnetic field changes by a single Barkhausen front jump from the first end to the second end or vice versa and where the response of the bistable magnetic wire is subsequently sensed by a sensing element, according to this invention, the nature of which lies is that the excitation element and the bistable magnetic wire are maintained in a mutual position, in which the size of the magnetic field excited by the excitation element at the first end is different from the size of the magnetic field excited by the excitation element at the second end.
  • the magnetic field has a triangular shape, especially preferably a symmetrical triangular shape, and the time of the local maximum and the time of the local minimum of response of the bistable magnetic wire are evaluated, which are essentially the time points of magnetization of the bistable magnetic wire.
  • the sum of these times is a parameter that expresses the dependence of the measured quantity or position, wherein other unmeasured factors and noise are suppressed. This improves the interpretability of the measured data and also accelerates their evaluation. It is also suitable if the difference between these times is calculated and this parameter expresses the parasitic magnetic field, which interferes the measurement of conventional magnetic sensors.
  • the process according to this invention suppresses the effects of the parasitic magnetic field.
  • An important feature of both the system and the method according to this invention is the fact that in the evaluation of the response signal, the local maximums and minimums are searched, and after their recognition, we work with times T1, T2, at which these maximums and minimums were measured. Furthermore, the method does not work on the basis of the values of the measured amplitudes, as was common in the prior art, but works with the values of the times, which is an easily and clearly identifiable parameter in the received signals. Thanks to that evaluation fast, accurate and insensitive to various secondary effects. For example, the exact position, shape and size of the excitation and sensing elements are not important.
  • the method according to this invention comprises the step of exciting the magnetic field with a different or varying frequency according to the type of measured quantity or position.
  • the universal excitation generator as well as the excitation element will optionally be adapted to this, or various excitation elements will be used for various applications.
  • one construction of the bistable magnetic wire can also be used at different frequencies.
  • the stable frequency value for one application may differ from the stable frequency used in another application, or these frequencies may be variable in a range different for the particular type of measurement.
  • a significant advantage of the present invention is the repeatable accuracy of the measurements, which is related to the increase of the interpretation level of the obtained raw data. A rapid response to a change in the measured physical quantity was also demonstrated. Thanks to the small dimensions of the bistable magnetic wire, the low cost and its energetic passivity, the system according to this invention can be used in a wide range of technical applications.
  • the bistable magnetic wire 1 is used for measurement the tension, or the pressure in the steel part.
  • the tear pattern has a calibrated center zone and two clamping ends.
  • a micro wire with a metal core diameter of approx. 15 ⁇ m and with glass cover with a total diameter of approx. 45 ⁇ m with a length of approximately 3 cm are glued to the surface in the central zone.
  • the bistable magnetic wire 1 is oriented in the direction of the tension force, wherein the elongations of the steel material are transmitted to the deformation of the bistable magnetic wire 1. Slight mounting angular position deviations do not have a significant effect on the measurement accuracy.
  • the bistable magnetic wire 1 is at the same time essentially aligned in a straight line, where the first end 11 and the second end 12 are in a mutual opposite position, so that the bistable magnetic wire 1 is not wound on the core, as known from prior art applications.
  • the excitation element 2 is placed next to the bistable magnetic wire 1, the longitudinal axis of the excitation element 2 is essentially parallel to the longitudinal axis of the bistable magnetic wire 1, wherein the center of the coil of the excitation element 2 is moved with respect to the center of the bistable magnetic wire 1 by the value X recorded in figure 6 .
  • the longitudinal axis of the excitation element 2 and the longitudinal axis of the bistable magnetic wire 1 are placed in a position, where if we intersect one common plain through them, this common plain is essentially perpendicular to the surface of the steel part.
  • the measuring system is insensitive to the inaccuracies of the placement of the individual elements, it is only essential, that the elongations of the measured material are reliably transferred to the bistable magnetic wire 1.
  • the positional asymmetry of the excitation element 2 leads to the desired difference of the magnetic field at the first end 11 and at the second end 12, which together with the properties of the bistable magnetic wire 1 leads to magnetization by a single Barkhausen jump from the first end 11 to the second end 12.
  • the excitation element 2 generates a magnetic field with a triangular signal and the response of the bistable magnetic wire 1 is captured with a sensor element 3, which is connected to the control unit 4, where the response is evaluated.
  • the signal obtained in the sensing element 3 is overall monotonic and with a high repeated accuracy.
  • a heat-sensitive bistable magnetic wire 1 is placed on the cell surface.
  • the system also comprises a planar coil of the excitation element 2 and a smaller coil of the sensing element 3. The measurement was performed in the temperature range from -20 to +100 °C.
  • the analog signal from the bistable magnetic wire 2 in the form of two peaks (minimum and maximum) is monitored by an oscilloscope.
  • the position time of the signal peaks T1 (maximum) and T2 (minimum) is processed and transformed into a digital signal in the control unit 4 and is subsequently displayed on the PC.
  • the measured and evaluated signal shows an almost linear dependence between the temperature and the magnetic response of the bistable magnetic wire 1, which is defined by the sum of the values T1 + T2.
  • the parameters from the detected dependence were used to adjustment the parameters of the software that shows the actual temperature.
  • a calibration polynomial can be defined to be used to assign the raw data to the actual temperature.
  • the sampling frequency is 2 samples/second with a sensitivity of 0.4 °C (K), which corresponds to a 288-point change at 120 ° C interval.
  • bistable magnetic wire 1 which is connected to a moving piston, is used for measurement the linear position with high accuracy.
  • the bistable magnetic wire 1 in this example with the composition Fe 77.5 Si 7.5 Bis has a positive magnetostriction, has a length of 30 mm, a metal core diameter of 39 ⁇ m and a diameter with the glass layer of 71 ⁇ m.
  • the excitation element 2 and the sensing element 3 are formed by coils, which loosely surround the sliding piston.
  • the longitudinal axes of the excitation element 2, the sensing element 3 and the piston are identical.
  • the bistable magnetic wire 1 is mounted on the surface of the piston, so it has only an approximately coaxial position with the excitation element 2 and the sensing element 3, which, however, does not affect the accuracy of the position measurement.
  • the asymmetry of the magnetic field in this example is achieved by positional asymmetry, wherein in each position of the piston the center of the bistable magnetic wire 1 is placed outside of the center of the excitation element 2. Moreover, in this example applies, that also both ends 11, 12 are in each position placed outside of the center of the excitation element 2.
  • the position of the excitation element 2 is thus set so that at the end position of the piston, one end of the bistable magnetic wire 1 extends inside the coil of the excitation element 2, but does not reach the center of the excitation element 2. Subsequently, the piston with the bistable magnetic wire 1 extends even more from the inside of the coil of the excitation element 2.
  • the system according to this example detects the magnetization proportional to the position of the bistable magnetic wire 1.
  • a reliable induction method is used for detection of magnetization.
  • the excitation field has a triangular shape and the switching time is measured, where T1 and T2 express the magnetization time (positive and negative switching) between the two stable magnetic states according to figure 10 .
  • the switching time corresponds to the time when the maximum voltage is induced.
  • the maximum and minimum of the received signal can be clearly identified, the background does not affect the interpretation possibilities.
  • the correctly amplified and filtered sensed signal is connected to the digital input of a single-chip computer with a time resolution of within 10 ns.
  • the simple electronics in the control unit 4 is sufficient to achieve very high accuracy and measurement speed.
  • the digital unit of the microcontroller generates a PWM signal of the desired frequency, in this example 135 Hz. After filtering the received signal and transforming it, the times T1 + T2 are sum up by a timer.
  • the advantage of the system according to this example is the sharp maximum of the signal induced during the magnetization and the high sensitivity at the level of 10 ⁇ m.
  • the system is also independent of the ambient temperature, the measurement error due to temperature sensitivity is less than 0.19%.
  • the coil of the excitation element 2 is wound unevenly so that it has an increased number of threads at one end.
  • the bistable magnetic wire 1 is positioned so that at a given time of non-zero excitation, the size of the magnetic field excited by the excitation element 2 at the first end 11 is at least 5% different from the size of the magnetic field excited by the excitation element 2 on the second end 12.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Magnetic Variables (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
EP22166892.4A 2022-04-06 2022-04-06 System zur messung einer physikalischen grösse und/oder positionsmesssystem mit bistablem magnetdraht sowie messverfahren Pending EP4257929A1 (de)

Priority Applications (2)

Application Number Priority Date Filing Date Title
EP22166892.4A EP4257929A1 (de) 2022-04-06 2022-04-06 System zur messung einer physikalischen grösse und/oder positionsmesssystem mit bistablem magnetdraht sowie messverfahren
PCT/IB2023/053187 WO2023194852A1 (en) 2022-04-06 2023-03-30 Physical quantity measurement system and/or for position measurement with bistable magnetic wire, method of measurement

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Application Number Priority Date Filing Date Title
EP22166892.4A EP4257929A1 (de) 2022-04-06 2022-04-06 System zur messung einer physikalischen grösse und/oder positionsmesssystem mit bistablem magnetdraht sowie messverfahren

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EP4257929A1 true EP4257929A1 (de) 2023-10-11

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EP22166892.4A Pending EP4257929A1 (de) 2022-04-06 2022-04-06 System zur messung einer physikalischen grösse und/oder positionsmesssystem mit bistablem magnetdraht sowie messverfahren

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Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2817169A1 (de) 1978-04-20 1979-10-31 Bosch Gmbh Robert Einrichtung zur abgabe von impulsen
GB2071336A (en) * 1980-03-06 1981-09-16 Duerrwaechter E Dr Doduco Induction-Type Position Encoder
GB2073428A (en) * 1980-03-06 1981-10-14 Doduco E A switching arrangement for the digital remote transmission of signals
US4484090A (en) 1980-02-22 1984-11-20 Echlin Manufacturing Company Pulse generator with shaped magnetic field
DE3427582A1 (de) 1984-07-26 1986-02-20 Doduco KG Dr. Eugen Dürrwächter, 7530 Pforzheim Verfahren zum ausloesen von wiegand-impulsen
JPH03252577A (ja) 1990-03-02 1991-11-11 Unitika Ltd 磁界検出法および磁界センサ
EP0484716A1 (de) 1990-11-09 1992-05-13 Vacuumschmelze GmbH Elektromagnetischer Geber zur Bestimmung der Drehzahl und/oder Drehrichtung eines Rotors
SU1753425A1 (ru) 1990-12-10 1992-08-07 Ленинградский электротехнический институт им.В.И.Ульянова (Ленина) Устройство дл определени параметров вращени
DE4107847C1 (en) 1991-03-12 1992-09-24 Mercedes-Benz Aktiengesellschaft, 7000 Stuttgart, De Impulse sensor using Wiegand effect - has winding connected to single pole switch for short circuiting winding when physical quantity e.g. temp., pressure, acceleration etc. changes
US6084400A (en) * 1994-03-07 2000-07-04 Amb Gmbh Angle of rotation sensor having a counting arrangement with at least two pulser-wire motion sensors providing electrical energy used as a voltage supply
GB2374084A (en) 2001-04-03 2002-10-09 Fourwinds Group Inc Alloys having bistable magnetic behaviour

Patent Citations (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2817169A1 (de) 1978-04-20 1979-10-31 Bosch Gmbh Robert Einrichtung zur abgabe von impulsen
US4484090A (en) 1980-02-22 1984-11-20 Echlin Manufacturing Company Pulse generator with shaped magnetic field
GB2071336A (en) * 1980-03-06 1981-09-16 Duerrwaechter E Dr Doduco Induction-Type Position Encoder
GB2073428A (en) * 1980-03-06 1981-10-14 Doduco E A switching arrangement for the digital remote transmission of signals
DE3427582A1 (de) 1984-07-26 1986-02-20 Doduco KG Dr. Eugen Dürrwächter, 7530 Pforzheim Verfahren zum ausloesen von wiegand-impulsen
JPH03252577A (ja) 1990-03-02 1991-11-11 Unitika Ltd 磁界検出法および磁界センサ
EP0484716A1 (de) 1990-11-09 1992-05-13 Vacuumschmelze GmbH Elektromagnetischer Geber zur Bestimmung der Drehzahl und/oder Drehrichtung eines Rotors
SU1753425A1 (ru) 1990-12-10 1992-08-07 Ленинградский электротехнический институт им.В.И.Ульянова (Ленина) Устройство дл определени параметров вращени
DE4107847C1 (en) 1991-03-12 1992-09-24 Mercedes-Benz Aktiengesellschaft, 7000 Stuttgart, De Impulse sensor using Wiegand effect - has winding connected to single pole switch for short circuiting winding when physical quantity e.g. temp., pressure, acceleration etc. changes
US6084400A (en) * 1994-03-07 2000-07-04 Amb Gmbh Angle of rotation sensor having a counting arrangement with at least two pulser-wire motion sensors providing electrical energy used as a voltage supply
GB2374084A (en) 2001-04-03 2002-10-09 Fourwinds Group Inc Alloys having bistable magnetic behaviour

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WO2023194852A1 (en) 2023-10-12

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